Diemer Peter J, Hayes Jacori, Welchman Evan, Hallani Rawad, Pookpanratana Sujitra J, Hacker Christina A, Richter Curt A, Anthony John E, Thonhauser Timo, Jurchescu Oana D
Department of Physics, Wake Forest University, Winston-Salem, NC 27109, USA.
Department of Chemistry, University of Kentucky, Lexington, KY 40506, USA.
Adv Funct Mater. 2017 Jan;3(1). doi: 10.1002/aelm.201600294. Epub 2016 Dec 14.
Organic field-effect transistor (OFET) performance is dictated by its composition and geometry, as well as the quality of the organic semiconductor (OSC) film, which strongly depends on purity and microstructure. When present, impurities and defects give rise to trap states in the bandgap of the OSC, lowering device performance. Here, 2,8-difluoro-5,11-bis(triethylsilylethynyl)-anthradithiophene is used as a model system to study the mechanism responsible for performance degradation in OFETs due to isomer coexistence. The density of trapping states is evaluated through temperature dependent current-voltage measurements, and it is discovered that OFETs containing a mixture of - and -isomers exhibit a discrete trapping state detected as a peak located at ~ 0.4 eV above the valence-band edge, which is absent in the samples fabricated on single-isomer films. Ultraviolet photoelectron spectroscopy measurements and density functional theory calculations do not point to a significant difference in electronic band structure between individual isomers. Instead, it is proposed that the dipole moment of the -isomer present in the host crystal of the -isomer locally polarizes the neighboring molecules, inducing energetic disorder. The isomers can be separated by applying gentle mechanical vibrations during film crystallization, as confirmed by the suppression of the peak and improvement in device performance.
有机场效应晶体管(OFET)的性能取决于其组成和几何形状,以及有机半导体(OSC)薄膜的质量,而这又很大程度上取决于纯度和微观结构。当存在杂质和缺陷时,它们会在OSC的带隙中产生陷阱态,从而降低器件性能。在此,2,8-二氟-5,11-双(三乙基硅乙炔基)-蒽并二噻吩被用作模型系统,以研究由于异构体共存导致OFET性能下降的机制。通过温度依赖的电流-电压测量来评估陷阱态密度,结果发现,含有α-和β-异构体混合物的OFET表现出一种离散的陷阱态,表现为位于价带边缘上方约0.4 eV处的一个峰值,而在单异构体薄膜制备的样品中不存在该峰值。紫外光电子能谱测量和密度泛函理论计算并未表明各个异构体之间的电子能带结构存在显著差异。相反,有人提出,α-异构体主体晶体中存在的β-异构体的偶极矩会使相邻分子局部极化,从而引发能量无序。通过在薄膜结晶过程中施加轻柔的机械振动可以分离异构体,这一点通过峰值的抑制和器件性能的改善得到了证实。